NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = T.Weber Found 68 matches. 2008MA33 Bull.Rus.Acad.Sci.Phys. 72, 806 (2008) A.I.Mazur, A.M.Shirokov, J.P.Vary, T.A.Weber, E.A.Mazur Charge-dependent NN interaction in the J-matrix inverse scattering approach
doi: 10.3103/S1062873808060208
2008SH16 Phys.Atomic Nuclei 71, 1232 (2008); Yad.Fiz. 71, 1260 (2008) A.M.Shirokov, J.P.Vary, A.I.Mazur, T.A.Weber Spectroscopy of light nuclei with realistic NN interaction JISP NUCLEAR STRUCTURE 3H, 3,4,6He, 6,7Li, 7,8,9,10Be, 9,10,11,12,13B, 10,11,12,13,14C, 12,13,14,15N, 13,14,15,16O; calculated binding energies using bare and effective interaction; 6Li, 10B; calculated rms radii, ground state quadrupole moments, ground and excited state energies; 10B; calculated B(E2) and B(GT) transition strengths; microscopic no-core shell model; realistic NN interaction.
doi: 10.1134/S1063778808070168
2007BO39 At.Data Nucl.Data Tables 93, 831 (2007) J.B.Boffard, B.Chiaro, T.Weber, C.C.Lin Electron-impact excitation of argon: Optical emission cross sections in the range of 300-2500 nm ATOMIC PHYSICS Ar(e, e'), E=25, 50, 100 eV; measured cross sections and excitation functions.
doi: 10.1016/j.adt.2007.06.004
2007MA49 Bull.Rus.Acad.Sci.Phys. 71, 754 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 781 (2007) A.I.Mazur, A.M.Shirokov, J.P.Vary, T.A.Weber, S.A.Zaitsev, E.A.Mazur Nonlocal nucleon-nucleon interaction JISP
doi: 10.3103/S1062873807060020
2007SH27 Bull.Rus.Acad.Sci.Phys. 71, 764 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 791 (2007) A.M.Shirokov, J.P.Vary, A.I.Mazur, T.A.Weber Nonlocal inverse-scattering nucleon-nucleon interaction and spectra of s- and p-shell nuclei NUCLEAR STRUCTURE H, He, Li, Be, B, C, N, O; calculated binding energies using no-core shell-model.
doi: 10.3103/S1062873807060032
2007SH52 Phys.Lett. B 644, 33 (2007) A.M.Shirokov, J.P.Vary, A.I.Mazur, T.A.Weber Realistic nuclear Hamiltonian: Ab exitu approach NUCLEAR STRUCTURE 3H, 3,4He, 6He, 6,7Li, 7,8,9,10Be, 9,10,11,12B, 10,11,12,13,14C, 12,13,14,15N, 13,14,15,16O; calculated binding energies with bare JISP16 and effective interaction generated by JISP16, ground and excitation energies. Fully-microscopic no-core shell model (NCSM).
doi: 10.1016/j.physletb.2006.10.066
2006EL07 Eur.Phys.J. A 28, Supplement 1, 197 (2006) M.El-Ghazaly, H.Backe, W.Lauth, G.Kube, P.Kunz, A.Sharafutdinov, T.Weber X-ray phase contrast imaging at MAMI
doi: 10.1140/epja/i2006-09-021-6
2006LA21 Eur.Phys.J. A 28, Supplement 1, 185 (2006) W.Lauth, H.Backe, O.Kettig, P.Kunz, A.Sharafutdinov, T.Weber Coherent X-rays at MAMI
doi: 10.1140/epja/i2006-09-019-0
2005SH31 Phys.Lett. B 621, 96 (2005) A.M.Shirokov, J.P.Vary, A.I.Mazur, S.A.Zaytsev, T.A.Weber Novel NN interaction and the spectroscopy of light nuclei NUCLEAR STRUCTURE 2H; calculated binding energy, radius, quadrupole moment. 3H, 3,4,6He, 6Li; calculated binding energies. 6He, 6Li; calculated excited states energies, radii, quadrupole moments. Inverse scattering potential.
doi: 10.1016/j.physletb.2005.06.043
2005SH33 J.Phys.(London) G31, S1283 (2005) A.M.Shirokov, J.P.Vary, A.I.Mazur, S.A.Zaytsev, T.A.Weber NN potentials from the J-matrix inverse scattering approach NUCLEAR STRUCTURE 2,3H, 3,4,6He, 6Li; calculated binding energies. 2H calculated radius, D-state probability. 6He, 6Li; calculated excited states energies, radii, quadrupole moments.
doi: 10.1088/0954-3899/31/8/006
2005VA32 Eur.Phys.J. A 25, Supplement 1, 475 (2005) J.P.Vary, O.V.Atramentov, B.R.Barrett, M.Hasan, A.C.Hayes, R.Lloyd, A.I.Mazur, P.Navratil, A.G.Negoita, A.Nogga, W.E.Ormand, S.Popescu, B.Shehadeh, A.M.Shirokov, J.R.Spence, I.Stetcu, S.Stoica, T.A.Weber, S.A.Zaytsev Ab initio No-Core Shell Model -- Recent results and future prospects NUCLEAR STRUCTURE 4He; calculated radius. 6Li, 16O, 48Ar, 48K, 48Ca, 48Sc, 48Ti, 48V, 48Cr, 48Mn; calculated ground-state energies. 16O, 47Ca; calculated excited states energies. No-core shell model.
doi: 10.1140/epjad/i2005-06-214-x
2004SC25 Nucl.Phys. A737, 306 (2004) H.Schmidt-Bocking, R.Dorner, O.Jagutzki, T.Jahnke, V.Mergel, L.Ph.H.Schmidt, Th.Weber, A.Czasch, Ch.Wimmer, M.Hattass, A.Knapp, M.Schoffler, C.L.Cocke, M.Prior, A.Kheifets, E.Weigold, F.Afaneh Many-particle dynamics in atomic and molecular physics investigated with the COLTRIMS-technique: New inside into e-e- correlation
doi: 10.1016/j.nuclphysa.2004.03.093
2004SH41 Phys.Rev. C 70, 044005 (2004) A.M.Shirokov, A.I.Mazur, S.A.Zaytsev, J.P.Vary, T.A.Weber Nucleon-nucleon interaction in the J-matrix inverse scattering approach and few-nucleon systems NUCLEAR REACTIONS 1H(n, n), E=0-350 MeV; calculated phase shifts. No-core shell model, J-matrix version of inverse scattering theory. NUCLEAR STRUCTURE 2,3H, 4He; calculated ground-state energies, radii. 4He calculated excited states energies. No-core shell model, J-matrix version of inverse scattering theory.
doi: 10.1103/PhysRevC.70.044005
2002SH36 Bull.Rus.Acad.Sci.Phys. 65, 1709 (2002) A.M.Shirokov, J.P.Vary, T.A.Weber, A.I.Mazur Realistic NN-Interaction in Shell Model NUCLEAR STRUCTURE 2H; calculated wave function. 3H, 4He; calculated ground-state energies vs model parameters. Phase-equivalent transformations.
2000GA03 Nucl.Phys. A662, 235 (2000) P.E.Garrett, H.Baltzer, M.Bertschy, D.G.Burke, M.Deleze, S.Drissi, C.Gunther, J.Jolie, J.Kern, H.Lehmann, S.J.Mannanal, J.Manns, U.Muller, J.P.Vorlet, N.Warr, T.Weber Nuclear Levels in 190Ir Studied with the 192Os(p, 3nγ) and 192Os(d, 4ne-) Reactions NUCLEAR REACTIONS 192Os(p, 3n), E=18.6, 20.8, 24.2, 27.2, 31.1 MeV; measured Eγ, Iγ(t), γγ-coin. 192Os(d, 4n), E=27.8 MeV; measured E(ce), I(ce), e-e--coin. 190Ir deduced levels J, π, T1/2. Two-quasiparticle-rotor calculations. Enriched targets, Ge detectors, orange spectrometers. NUCLEAR STRUCTURE 189Os, 190,191Ir; calculated levels, J, π. Particle-rotor calculations.
doi: 10.1016/S0375-9474(99)00365-6
1999KH01 J.Phys.(London) B32, L73 (1999) Kh.Khayyat, T.Weber, R.Dorner, M.Achler, V.Mergel, L.Spiedlberger, O.Jagutzki, U.Meyer, J.Ullrich, R.Moshammer, W.Schmitt, H.Knudsen, U.Mikkelsen, P.Aggerholm, E.Uggerhoej, S.P.Moeller, V.D.Rodriguez, S.F.C.O'Rourke, R.E.Olson, P.D.Fainstein, J.H.McGuire, H.Schmidt-Bocking Differential Cross Sections in Antiproton- and Proton-Helium Collisions ATOMIC PHYSICS 4He(p-bar, p-bar), (p, p), E ≈ 1 MeV; measured recoil momentum following ionization.
doi: 10.1088/0953-4075/32/4/002
1999WU05 Acta Phys.Pol. B30, 1313 (1999) M.Wurkner, J.De Boer, J.Choinski, T.Czosnyka, C.Droste, C.Gunther, J.Iwanicki, M.Kisielinski, A.Kordyasz, M.Kowalczyk, H.Kusakari, J.Kvasil, A.I.Levon, M.Loewe, P.J.Napiorkowski, T.Shizuma, G.Sletten, J.Srebrny, M.Sugawara, T.Weber, Y.Yoshizawa Coulomb Excitation of 231Pa NUCLEAR REACTIONS 231Pa(32S, 32S'), E=148 MeV; 231Pa(58Ni, 58Ni'), E=255, 260, 261 MeV; measured Eγ, Iγ(θ), (particle)γγ-coin following Coulomb excitation. 231Pa deduced high-spin levels, J, π. Nordball array.
1998MA83 Eur.Phys.J. A 3, 263 (1998) J.Manns, J.Groger, C.Gunther, U.Muller, T.Weber, J.de Boer Study of 227Th in the 226Ra(α, 3n) Reaction NUCLEAR REACTIONS 226Ra(α, 3n), E=33 MeV; measured Eγ, Iγ, E(ce), I(ce), γγ-, (ce)γ-coin. 227Th deduced high-spin levels, J, π, rotational bands, B(E1)/B(E2).
doi: 10.1007/s100500050176
1998WE01 Eur.Phys.J. A 1, 39 (1998) T.Weber, J.Groger, C.Gunther, J.deBoer Study of the First-Excited K(π) = 0+ and 2+ Bands in 228Th in the 226Ra(α, 2n) Reaction NUCLEAR REACTIONS 226Ra(α, 2n), E=28 MeV; measured Eγ, Iγ, (ce)γ-coin. 228Th deduced high-spin levels, J, π, vibrational bands.
doi: 10.1007/s100500050029
1998WE13 Eur.Phys.J. A 3, 25 (1998) T.Weber, J.de Boer, K.Freitag, J.Groger, C.Gunther, P.Herzog, V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Nuclear Levels in 228Th Populated in the Decay of 228Pa (II) RADIOACTIVITY 228Pa(EC); measured Eγ, Iγ, γγ-coin. 228Th deduced levels, J, π, δ, B(E2), rotational bands. NUCLEAR STRUCTURE 228Th; calculated levels J, π, transition strengths. Quasiparticle-phonon model.
doi: 10.1007/s100500050146
1997MU08 Phys.Rev. C55, 2267 (1997) U.Muller, P.Sevenich, K.Freitag, C.Gunther, P.Herzog, G.D.Jones, C.Kliem, J.Manns, T.Weber, B.Will, and the ISOLDE Collaboration Level Structure of 227Th Investigated in the α Decay of 231U RADIOACTIVITY 231U(α) [from 232Th(α, 5n), E=53 MeV]; measured Eα, Iα, Eγ, Iγ. 227Ac(β-); 227Th(α) [from 227Ac(β-decay)]; 223Ra(α) [from 227Th(α-decay)]; measured αγ-coin, I(ce), Eα, Iα, oriented nuclei. 227Th deduced levels, J, π, γ-multipolarity, α hindrance factors, reduced transition rates, octupole deformation.
doi: 10.1103/PhysRevC.55.2267
1997WE05 Z.Phys. A358, 281 (1997) T.Weber, J.deBoer, K.Freitag, J.Groger, C.Gunther, J.Manns, U.Muller Variety of Vibrational Excitations in 228Th RADIOACTIVITY 228Pa(EC); measured γγ-coin. 228Th deduced levels, J, π, K, band structure, moments of inertia.
doi: 10.1007/s002180050330
1996AC01 Z.Phys. A355, 151 (1996) B.Ackermann, Ch.Fleischmann, H.Baltzer, J.de Boer, T.Czosnyka, C.Gunther, U.Muller, T.Weber Investigation of Vibrational Levels in 226Ra by Coulomb Excitation and by the 226Ra(d, pnγ) Reaction NUCLEAR REACTIONS 226Ra(d, np), E=27 MeV; measured γ(ce)-coin. 226Ra(16O, 16O'), E=63 MeV; 226Ra(32S, 32S'), E=135 MeV; measured γ(scattered particle)-coin following Coulomb excitation. 226Ra deduced levels, J, π, K, B(λ), ratios, band structure.
doi: 10.1007/s002180050092
1996BA67 Z.Phys. A356, 13 (1996) H.Baltzer, J.deBoer, A.Gollwitzer, G.Graw, C.Gunther, A.I.Levon, M.Loewe, H.J.Maier, J.Manns, U.Muller, B.D.Valnion, T.Weber, M.Wurkner Study of Low-Lying 0+ Excitations in 228Th and 232,234,236U in the (p, t) Reaction NUCLEAR REACTIONS 230,232Th, 234,236,238U(p, t), E=22 MeV; measured triton spectra; deduced relative σ. 228,230Th, 232,234,236U deduced levels, J, π, K.
doi: 10.1007/s002180050142
1996GA30 Nucl.Phys. A611, 68 (1996) P.E.Garrett, N.Warr, H.Baltzer, S.Boehmsdorff, D.G.Burke, M.Deleze, S.Drissi, J.Groger, C.Gunther, J.Kern, S.J.Mannanal, J.Manns, U.Muller, J.-P.Vorlet, T.Weber Long-Lived Isomers in 190Ir NUCLEAR REACTIONS 192Os(p, 3n), E=18.6-31.1 MeV; 192Os(d, 4n), E=27.8 MeV; measured Eγ, Iγ vs Ep, (e-e-)-, (eγ)-coin. 190Ir deduced isomers T1/2, J, π, ICC, γ multipolarity. Enriched targets, Ge detector, β-ray spectrometer. RADIOACTIVITY 190mIr [from 192Os(p, 3n), E=18.6-31.1 MeV]; 192Os(d, 4n), E=27.8 MeV; measured Eγ, Iγ, I(ce), (e-e-)-, (e-γ)-coin, T1/2; deduced log ft. Enriched targets, Ge detector, β-ray spectrometer.
doi: 10.1016/S0375-9474(96)00330-2
1996LE01 Nucl.Phys. A598, 11 (1996) A.I.Levon, J.de Boer, G.Graw, J.Kvasil, M.Loewe, B.D.Valnion, M.Wurkner, H.Baltzer, C.Gunther, J.Manns, U.Muller, T.Weber The Structure of the Parity-Doublet Bands in 231Pa NUCLEAR REACTIONS 231Pa(d, d'), E=27 MeV; measured Ed. 231Pa(p, p'), E=11 MeV; measured Ep. 232Th(p, 2n), E=14 MeV; analyzed data. 231Pa(16O, 16O'), E=85 MeV; 231Pa(32S, 32S'), E=145 MeV; measured Eγ, Iγ following Coulomb excitation. 231Pa deduced levels, J, π, rotational bands, octupole correlations. Q3D magnetic spectrometer, Ge detectors. RADIOACTIVITY 231U(EC); measured I(ce), (e-γ)-, (e-e-)-coin. 231Pa deduced levels, J, π, band structure, γ-multipolarity, γ-branching ratio. Orange spectrometers, Ge detectors, enriched radioactive targets, mass-separated radioactive sources.
doi: 10.1016/0375-9474(95)00508-0
1995BA42 Z.Phys. A352, 47 (1995) H.Baltzer, K.Freitag, C.Gunther, P.Herzog, J.Manns, U.Muller, R.Paulsen, P.Sevenich, T.Weber, B.Will Nuclear Levels in 228Th Populated in the Decay of 228Pa RADIOACTIVITY 228Pa(EC) [from 232Th(p, 5n), E=40 MeV]; measured Eγ, Iγ, (eγ)-coin, I(ce). 228Th deduced levels, J, π, K, band structure, Iγ, δ, B(λ) ratios, γ multipolarity. Low temperature source orientation.
doi: 10.1007/BF01292760
1994AC02 Z.Phys. A350, 13 (1994) B.Ackermann, H.Baltzer, K.Freitag, C.Gunther, P.Herzog, J.Manns, U.Muller, R.Paulsen, P.Sevenich, T.Weber, B.Will, J.de Boer, G.Graw, A.I.Levon, M.Loewe, A.Losch, E.Muller-Zanotti Experimental Investigation of Vibrational Excitations in 230Th RADIOACTIVITY 230Pa(β+), (EC), (β-) [from 232Th(p, 3n), E not given]; measured Eγ, Iγ, I(ce). 230Th levels deduced Iγ, γ-multipolarity. NUCLEAR REACTIONS 230Th(d, np), E=23 MeV; measured (ce)(ce)-, γ(ce)-coin. 232Th(p, t), E=22 MeV; measured σ(θ). 230Th deduced levels, J, π, K, γ-multipolarity, B(λ), high-spin band structure.
doi: 10.1007/BF01285047
1994BO27 Nucl.Instrum.Methods Phys.Res. B85, 188 (1994) Consequence of the Fractal Nature of the Collision Cascade: End-of-range spikes in ballistic systems NUCLEAR REACTIONS Ti, N(α, α), E=900 keV; measured Rutherford backscattering spectra; deduced end of ion range spike formation features. Noble gas implantation of TiN on steel, Al.
doi: 10.1016/0168-583X(94)95811-4
1994OS06 Nucl.Instrum.Methods Phys.Res. B85, 499 (1994) T.Osipowicz, S.C.Liew, K.K.Loh, I.Orlic, S.M.Tang, Th.Weber Reconstruction of Ar Depth Profiles from PIXE Measurements NUCLEAR REACTIONS Ar(α, X), E=1.5, 1.3 MeV; measured X-ray yields, Ar implantation on Al samples; deduced Ar depth profiles reconstruction.
doi: 10.1016/0168-583X(94)95871-8
1991WE03 Nucl.Phys. A522, 443 (1991) Th.Weber, U.Kneissl, W.Pecho, A.Degener, K.Huber, K.Schaschek, W.Wilke Fragment Angular Distributions in Electron- and Positron-Induced Fission of 232Th. A Specific Test of Virtual Photon Spectra NUCLEAR REACTIONS 232Th(e, F), E=8-16 MeV; measured fission fragment σ(θ); deduced angular correlation coefficients, fission channels. Virtual photon spectra tests.
doi: 10.1016/0375-9474(91)90075-H
1990HE03 Nucl.Phys. A506, 223 (1990) R.D.Heil, B.Kasten, W.Scharfe, P.A.Butler, H.Friedrichs, S.D.Hoblit, U.Kneissl, S.Lindenstruth, M.Ludwig, G.Muller, H.H.Pitz, K.W.Rose, M.Schumacher, U.Seemann, J.Simpson, P.von Brentano, Th.Weber, C.Wesselborg, A.Zilges Parity Assignments in Nuclear Resonance Fluorescence Experiments Using Compton Polarimeters NUCLEAR REACTIONS 142,150Nd, 232Th(γ, γ'), E=4.1 MeV bremsstrahlung; measured Eγ, Iγ, asymmetry, linear polarization. 142,150Nd, 232Th deduced levels, J, π, Γ0, (Γ0)2/Γ0.
doi: 10.1016/0375-9474(90)90384-X
1990WE07 Nucl.Phys. A510, 1 (1990) Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, Th.Kihm, K.T.Knopfle, H.J.Emrich (e, e'f) Coincidence Experiments on 235U and 238U NUCLEAR REACTIONS 235,238U(e, e'F), E=78-183 MeV; measured σ(θ(e'), E, θ(fragment)), in-, out-of-plane fission fragment σ(θ), fragment time-of-flight differences. 235,238U deduced multipole strength distributions for giant E0, E1, E2, E3 resonances, fission characteristics.
doi: 10.1016/0375-9474(90)90286-U
1990WI15 Phys.Rev. C42, 2148 (1990) W.Wilke, U.Kneissl, Th.Weber, H.Stroher, L.S.Cardman, P.T.Debevec, S.D.Hoblit, R.T.Jones, A.M.Nathan Photofission of 238U with Monochromatic Gamma Rays in the Energy Range 11-16 MeV NUCLEAR REACTIONS 238U(γ, F), E=11-16 MeV; measured fission fragment σ(θ), fragment mass distributions; deduced anisotropy, fragment mass asymmetry relationship.
doi: 10.1103/PhysRevC.42.2148
1989KA16 Phys.Rev.Lett. 63, 609 (1989); Erratum Phys.Rev.Lett. 63, 2695 (1989) B.Kasten, R.D.Heil, P.v.Brentano, P.A.Butler, S.D.Hoblit, U.Kneissl, S.Lindenstruth, G.Muller, H.H.Pitz, K.W.Rose, W.Scharfe, M.Schumacher, U.Seemann, Th.Weber, C.Wesselborg, A.Zilges Evidence for a Cluster of Collective 1+ States in 150Nd Near 3 MeV NUCLEAR REACTIONS 150Nd(γ, γ'), E=2.8-3.1 MeV bremsstrahlung; measured Eγ, Iγ, γ linear polarization, asymmetry. 150Nd deduced levels, J, π, B(λ), (Γ02/Γ). Compton polarimeters.
doi: 10.1103/PhysRevLett.63.609
1989WE01 Phys.Rev.Lett. 62, 129 (1989) Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle Evidence for Different Mass Splits in Fission Decays of Giant Multipole Resonances from 235,238U(e, e'f) Reactions NUCLEAR REACTIONS 235,238U(e, e'F), E=185 MeV; measured fission (fragment)(fragment)-coin. 235,238U deduced giant multipole resonance fission decay features, Γ(S)/Γ(A).
doi: 10.1103/PhysRevLett.62.129
1989WE02 Phys.Rev.Lett. 62, 690 (1989) Th.Weber, U.Kneissl, Th.Kihm, K.T.Knopfle Weber et al. Reply
doi: 10.1103/PhysRevLett.62.690
1989WE12 Nucl.Phys. A502, 279c (1989) Th.Weber, W.Wilke, H.J.Emrich, R.D.Heil, Th.Kihm, U.Kneissl, K.T.Knopfle, U.Seemann, F.Steiper, H.Stroher Evidence for Different Fission Fragment Mass Asymmetries for Specific Nuclear Excitations Studied in (e, e'F) and (γ, F) Reactions NUCLEAR REACTIONS 236U(e, e'F), E not given; measured fission fragment σ(θ). 235,238U(e, e'F), E=185 MeV; measured fission fragment spectra; deduced symmetric, asymmetric fission yield ratios, excitation multipolarity role.
doi: 10.1016/0375-9474(89)90668-4
1988WE18 Phys.Lett. 215B, 469 (1988) Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle Near Barrier Fission Channels (J(π), K) in 238U for Spins J(π) = 0+, 1-, and 2+ from (e, e'f) Angular Correlation Measurements NUCLEAR REACTIONS 238U(e, e'F), E=185 MeV; measured fission (fragment)(fragment)(θ), in-plane, out-of-plane; deduced partial fission channel σ. 238U levels deduced fission barriers.
doi: 10.1016/0370-2693(88)91343-3
1988WI15 Phys.Lett. 207B, 385 (1988) W.Wilke, R.D.Heil, U.Kneissl, U.Seemann, F.Steiper, H.Stroher, T.Weber Angular Distributions of Photofission Fragments of Particular Mass NUCLEAR REACTIONS 236U(γ, F), E=16 MeV bremsstrahlung; measured fission fragment σ(θ), mass distribution. 236U deduced fission mechanism.
doi: 10.1016/0370-2693(88)90669-7
1988WI20 Nucl.Instrum.Methods Phys.Res. A272, 785 (1988) W.Wilke, H.Bruckel, R.D.Heil, U.Kneissl, H.Stroher, Th.Weber A 4π Double Obelisk of Position Sensitive PPACs for New Vistas in Photofission Experiments NUCLEAR REACTIONS 238U(γ, F), E=5.6-16 MeV bremsstrahlung; measured fission fragment spectra, σ(θ), mass distribution. Position sensitive detectors, 4π array.
doi: 10.1016/0168-9002(88)90760-7
1987WE09 Phys.Rev.Lett. 59, 2028 (1987) Th.Weber, R.D.Heil, U.Kneissl, W.Pecho, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle Multipole Strength Distributions and Form Factors for E1, E2/E0, and E3 from 238U(e, e'f) Coincidence Experiments NUCLEAR REACTIONS 238U(e, e'F), E=78, 183, 124 MeV; measured fission (fragment)(fragment)-coin. 238U deduced multipole strength distributions, form factors.
doi: 10.1103/PhysRevLett.59.2028
1987WI15 Nucl.Phys. A473, 129 (1987) Ch.Winter, B.Krusche, K.P.Lieb, T.Weber, G.Hlawatsch, T.von Egidy, F.Hoyler Spectroscopy of 88Sr with the 87Sr(n, γ) and 87Sr(d, p) Reactions NUCLEAR REACTIONS 87Sr(n, γ), E=thermal; measured Eγ, Iγ. 87Sr(d, p), E=20 MeV; measured σ(E(p)). 88Sr deduced levels, neutron binding energy, level density, γ transition strengths, branching ratios.
doi: 10.1016/0375-9474(87)90158-8
1985DR01 Nucl.Phys. A437, 253 (1985) J.Drexler, R.D.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, T.Weber, W.Wilke, B.Fischer, H.Hollick The ' Isomeric Shelf ' in the Deep Subbarrier Photofission of 238U NUCLEAR REACTIONS 238U(γ, F), E=3.9-4.3 MeV bremsstrahlung; measured T1/2, isomeric to prompt yield ratio. Depleted targets.
doi: 10.1016/0375-9474(85)90087-9
1985HE21 Nucl.Instrum.Methods 239, 545 (1985) R.D.Heil, J.Drexler, K.Huber, U.Kneissl, G.Mank, H.Ries, H.Stroher, T.Weber, W.Wilke A Compact Time-of-Flight Spectrometer for Electrofission Studies RADIOACTIVITY 252Cf(SF); measured fission fragment velocities, masses, energies before neutron emission.
doi: 10.1016/0168-9002(85)90034-8
1984BE54 Phys.Lett. 149B, 59 (1984) U.E.P.Berg, C.Blasing, J.Drexler, R.D.Heil, U.Kneissl, W.Naatz, R.Ratzek, S.Schennach, R.Stock, T.Weber, H.Wickert, B.Fischer, H.Hollick, D.Kollewe Photoexcitation of Low-Lying Collective States in 156,158,160Gd NUCLEAR REACTIONS 156,158,160Gd(γ, γ'), E=2.8-3.4 MeV bremsstrahlung; measured Eγ, Iγ. 156,158,160Gd levels deduced Γγ, B(M1), transition collectivity.
doi: 10.1016/0370-2693(84)91551-X
1984CO06 Lett.Nuovo Cim. 39, 119 (1984) An Analysis for the Charge and Point Proton Distribution of 3He with Minimal Systematic Error NUCLEAR MOMENTS 3He(e, e), E not given; analyzed form factor data. 3He deduced charge, point proton distribution, method dependent error estimate.
doi: 10.1007/BF02800292
1984DR04 Nucl.Instrum.Methods 220, 409 (1984) J.Drexler, R.D.Fischer, R.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, H.Stroher, T.Weber, W.Wilke Arrangements of Parallel Plate Avalanche Detectors for Electrofission and Photofission experiments NUCLEAR REACTIONS 232Th(e+, F), (e-, F), E=9 MeV; measured fission fragment σ(θ). Parallel plate avalanche detectors. RADIOACTIVITY 252Cf(SF); measured fission fragment tof spectra. Parallel plate avalanche detectors.
doi: 10.1016/0167-5087(84)90303-X
1984RI08 Phys.Rev. C29, 2346 (1984) H.Ries, G.Mank, J.Drexler, R.Heil, K.Huber, U.Kneissl, R.Ratzek, H.Stroher, T.Weber, W.Wilke Absolute Photofission Cross Sections for 235,238U in the Energy Range 11.5-30 MeV NUCLEAR REACTIONS 238,235U(γ, F), E=11.5-30 MeV; measured absolute fission σ(E). Quasimonoenergetic photons from positron annihilation, multiple parallel plate detectors.
doi: 10.1103/PhysRevC.29.2346
1984ST07 Nucl.Phys. A419, 295 (1984) H.Stroher, J.Drexler, R.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, T.Weber, W.Wilke, H.J.Maier Fission Barriers of Preactinide Nuclei from Electrofission Experiments NUCLEAR REACTIONS 182,184,186W, Pt, 209Bi(e, F), E=25-55 MeV; measured electron induced fission σ(E); deduced fission barriers B. Natural, enriched targets. Statistical model analysis.
doi: 10.1016/0375-9474(84)90394-4
1984WE05 Z.Phys. A315, 125 (1984) T.Weber, J.Drexler, R.D.Heil, K.Huber, U.Kneissl, G.Mank, H.Ries, H.Stroher, W.Wilke A New Method to Test Virtual Photon Spectra NUCLEAR REACTIONS 232Th(e-, F), E=9 MeV; 232Th(e+, F), E=16 MeV; measured fission fragment σ(θ), anisotropy.
doi: 10.1007/BF01436220
1983DR14 Nucl.Phys. A411, 17 (1983) J.Drexler, R.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, H.Stroher, T.Weber, W.Wilke The Decay of Uranium Shape Isomers Investigated by Photonuclear Reactions NUCLEAR REACTIONS 238U(γ, γ'), E=12 MeV bremsstrahlung; measured isomer T1/2, isomeric to prompt yield ratio; deduced isomeric fission cross section. 238U deduced isomer decay branching ratio. Natural target.
doi: 10.1016/0375-9474(83)90505-5
1979BA54 Nucl.Instrum.Methods 163, 377 (1979) R.Bass, J.Idzko, H.Pelz, K.Stelzer, T.Weber, R.Weniger Symmetrical Four-Crystal Compton Polarimeter for Gamma Rays: Design and Application RADIOACTIVITY 24,25Mg, 152Eu, 56Co; measured asymmetry (Eγ). Four crystal Compton polarimeter. NUCLEAR REACTIONS 107,109Ag(α, α'γ), E=2.5 MeV; 28Si, Fe(p, p'γ), E=3.10 MeV; 24Mg(p, p'γ), E=2.01, 6.06 MeV; 31P(α, pγ), E=6.30, 7.00 MeV; measured linear polarization, polarization sensitivity. 36Ar(α, pγ), 92Zr(p, nγ), E not given; measured γ(θ), linear polarization P(θγ). 39K level deduced J, π, δ. 92Nb level deduced J, π ≠ 0-; four crystal Compton polarimeter.
doi: 10.1016/0029-554X(79)90122-8
1979GM02 Czech.J.Phys. B29, 155 (1979); Erratum Czech.J.Phys. B29, 1308 (1979) M.Gmitro, E.Tinkova, A.Rimini, T.Weber Positive Parity Giant Multipole Resonances in 16O NUCLEAR STRUCTURE 16O; calculated T=0, 1, GMR strength distribution for positive pariy J=0 to 4 states. Shell model n particle-n hole.
doi: 10.1007/BF01957544
1977GM01 Lett.Nuovo Cim. 20, 449 (1977) M.Gmitro, E.Tinkova, A.Rimini, T.Weber Spreading of the Giant Quadrupole Resonance in 16O NUCLEAR STRUCTURE 16O; calculated distribution of isoscalar GQR.
doi: 10.1007/BF02783557
1975BO19 Nuovo Cim. 25A, 503 (1975) RPA-Oriented Shell Model Study of 56Ni NUCLEAR STRUCTURE 56Ni; calculated levels, role of 3p-3h configuration.
doi: 10.1007/BF02820861
1974GM02 Nuovo Cim. 21A, 11 (1974) The Role of the 4p-4h Excitations in the Microscopic Description of 56Ni NUCLEAR STRUCTURE 56Ni; calculated levels.
doi: 10.1007/BF02731184
1973GA05 Phys.Rev. C7, 1454 (1973) Y.K.Gambhir, A.Rimini, T.Weber Analysis of (p, t) and (t, p) Reaction Data for Nickel Isotopes with Structure Wave Functions of the Broken-Pair Approximation NUCLEAR REACTIONS 58,60,62,64,66Ni(p, t), 58,60,62,64Ni(t, p); measured nothing; deduced S.
doi: 10.1103/PhysRevC.7.1454
1973GM01 Nuovo Cim. 13A, 526 (1973) On the n-n and n-p Effective Interactions for 1f7/2 Protons and (2p, 1f5/2) Neutrons NUCLEAR STRUCTURE 58,59,60Ni, 56,57Co, 55,56Fe, 54,55Mn, 53,54Cr; calculated levels, rms radii.
doi: 10.1007/BF02827353
1971GA06 Phys.Rev. C3, 1965 (1971) Y.K.Gambhir, A.Rimini, T.Weber Number-Conserving Shell-Model Calculations for Nickel and Tin Isotopes NUCLEAR STRUCTURE 58,60,62,64Ni, 116,120,124Sn; calculated levels. Number-conserving shell model.
doi: 10.1103/PhysRevC.3.1965
1970BO40 Lett.Nuovo Cim. 4, 988 (1970) Note on the Microscopic Description of the Charge Form Factor of 4He NUCLEAR STRUCTURE 4He; calculated charge form factor.
doi: 10.1007/BF02755259
1970BO43 Phys.Lett. 33B, 553 (1970) A.Boiti, M.Gmitro, A.Rimini, T.Weber On a Completely Microscopic Description of the 2p-1f Shell Nuclei NUCLEAR STRUCTURE 56Ni; calculated levels. Tamm-Dancoff, 2p-2h approximations.
doi: 10.1016/0370-2693(70)90346-1
1970GM01 Phys.Rev. C1, 1801 (1970) M.Gmitro, A.Rimini, P.Rossi, T.Weber Comparison between the Quasiparticle Tamm-Dancoff and Random-Phase Approximations in Even Tin Isotopes Using Realistic Interactions NUCLEAR STRUCTURE 116,120Sn; calculated levels. Quasiparticle Tamm-Dancoff, random phase approximations; realistic interactions.
doi: 10.1103/PhysRevC.1.1801
1970RI07 Phys.Rev. C2, 324 (1970) Effect of Particle-Number Projection on the Determination of the Ground State of Superconducting Nuclei NUCLEAR STRUCTURE 60,62,64Ni, 112,116,120,124Sn; calculated pair distribution coefficients for ground states. BCS, projected BCS theories.
doi: 10.1103/PhysRevC.2.324
1969AL08 Phys.Rev. 182, 1308 (1969) R.Alzetta, T.Weber, Y.K.Gambhir, M.Gmitro, J.Sawicki, A.Rimini Improved Inverse Gap Equation and Quasiparticle Theories of Odd and Even Tin Isotopes NUCLEAR STRUCTURE 115,116,117,118,119,120,121Sn; calculated levels, S for (d, p), (p, d), (d, t), (p, t) reactions. Quasiparticle theory, inverse gap equation.
doi: 10.1103/PhysRev.182.1308
1969AL16 Phys.Rev. 185, 1233 (1969) R.Alzetta, A.Rimini, T.Weber, M.Gmitro, J.Sawicki Effective N-N Interaction and Electromagnetic Operators Deduced from the Tabakin Potential: Application to Nickel Isotopes NUCLEAR STRUCTURE 58,59,60,61,62,63,64Ni; calculated levels, B(E2), B(M1). Second Tamm-Dancoff theory, Tabakin potential.
doi: 10.1103/PhysRev.185.1233
1968GM05 Phys.Rev. 175, 1243 (1968) M.Gmitro, A.Rimini, J.Sawicki, T.Weber Microscopic Theory of Effective Operators for Electromagnetic Interactions in Nuclei
doi: 10.1103/PhysRev.175.1243
1968RI04 Phys.Rev.Letters 20, 676 (1968) Inelastic Electron Scattering from Even Tin Isotopes and Microscopic Theories of Vibrational States
doi: 10.1103/PhysRevLett.20.676
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